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Table 4.

Best-fitting parameters for the four eROSITA epochs using the TBabs*apec model, and from the simultaneous fit to all XMM-Newton spectra using the TBabs*(apec+apec+apec) model.

Parameter eRASS1 eRASS2 eRASS3 eRASS4 XMM-Newton
NH [1020 cm−2] 3.4 (fixed) 3.4 (fixed) 3.4 (fixed) 3.4 (fixed) 3 . 4 0.2 + 0.3 $ 3.4^{+0.3}_{-0.2} $
kT1 [keV] 2 . 3 0.5 + 2.1 $ 2.3^{+2.1}_{-0.5} $ 13 5 + 29 $ 13^{+29}_{-5} $ 9 3 + 14 $ 9^{+14}_{-3} $ 4 . 8 0.9 + 1.3 $ 4.8^{+1.3}_{-0.9} $ 0.23 ± 0.01
kT2 [keV] 0 . 94 0.02 + 0.01 $ 0.94^{+0.01}_{-0.02} $
kT3 [keV] 5.2 ± 0.1
χ ν 2 ( ν ) $ \chi^{2}_{\nu}(\nu) $(a) 117.51(127) 0.88(22) 0.94(26) 0.83(16) 1.35(532)
Flux0.2 − 12 keV(b) [10−12 erg cm−2 s−1] 2.0 ± 0.2 17.4 ± 0.7 13.8 ± 0.5 6.1 ± 0.3 3.13 ± 0.01
Luminosity0.2 − 12 keV(c) [1032 erg s−1] 0.59 ± 0.05 5.1 ± 0.2 4.1 ± 0.2 1.79 ± 0.09 0.92 ± 0.02
Luminosity0.25 − 10 keV(c) [1032 erg s−1] 0.57 ± 0.05 4.7 ± 0.2 3.8 ± 0.2 1.71 ± 0.09 0.88 ± 0.01
Luminosity0.01 − 100 keV(c) [1032 erg s−1] 0.63 ± 0.06 5.3 ± 0.2 4.2 ± 0.2 1.9 ± 0.1 1.05 ± 0.02

Notes. Uncertainties are given at the 1σ confidence levels.

(a)

For eRASS1, the value corresponds to the C-statistic (d.o.f).

(b)

Unabsorbed fluxes.

(c)

Unabsorbed luminosities were estimated assuming a distance of 496 ± 4 pc.

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